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NSR database version of April 27, 2024.

Search: Author = J.Kopecky

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2020KA09      Nucl.Data Sheets 163, 109 (2020)

T.Kawano, Y.S.Cho, P.Dimitriou, D.Filipescu, N.Iwamoto, V.Plujko, X.Tao, H.Utsunomiya, V.Varlamov, R.Xu, R.Capote, I.Gheorghe, O.Gorbachenko, Y.L.Jin, T.Renstrom, M.Sin, K.Stopani, Y.Tian, G.M.Tveten, J.M.Wang, T.Belgya, R.Firestone, S.Goriely, J.Kopecky, M.Krticka, R.Schwengner, S.Siem, M.Wiedeking

IAEA Photonuclear Data Library 2019

doi: 10.1016/j.nds.2019.12.002
Citations: PlumX Metrics


2019GO30      Eur.Phys.J. A 55, 172 (2019)

S.Goriely, P.Dimitriou, M.Wiedeking, T.Belgya, R.Firestone, J.Kopecky, M.Krticka, V.Plujko, R.Schwengner, S.Siem, H.Utsunomiya, S.Hilaire, S.Peru, Y.S.Cho, D.M.Filipescu, N.Iwamoto, T.Kawano, V.Varlamov, R.Xu

Reference database for photon strength functions

doi: 10.1140/epja/i2019-12840-1
Citations: PlumX Metrics


2017KO20      Phys.Rev. C 95, 054317 (2017)

J.Kopecky, S.Goriely, S.Peru, S.Hilaire, M.Martini

E1 and M1 strength functions from average resonance capture data

NUCLEAR REACTIONS 75As, 91Zr, 95,97Mo, 101Ru, 105Pd, 113Cd, 123Te, 127I, 134,135Ba, 145Nd, 154Sm, 153Eu, 154,155,156,157,158Gd, 161,162,163,164Dy, 165Ho, 167Er, 169Tm, 171,173Yb, 175Lu, 177Hf, 181Ta, 183,184,186W, 187,188,190,192Os, 192,194Ir, 194,195,196,198Pt, 197Au, 232Th, 238U, 239Pu(n, γ), E=2, 24 keV; analyzed average resonance capture (ARC) data measured at different filter beam facilities ANL, INEL, and BNL between 1970 and 1990; deduced E1 and M1 photon strength function, comparison to the photon strength function extracted from other experimental methods, such as photoneutron data and Oslo-method data, and with quasiparticle random phase approximation (QRPA) calculations based on the D1M Gogny force.

doi: 10.1103/PhysRevC.95.054317
Citations: PlumX Metrics


2011PA30      J.Korean Phys.Soc. 59, 1100s (2011)

L.W.Packer, J.-Ch.Sublet, J.Kopecky, R.A.Forrest

Recent Progress in Neutron-, Proton- and Deuteron-induced Reaction Nuclear Data for EAF-2010 and the European Activation System

COMPILATION A=20-256(n, p), (n, α), E not given; compiled, compared EAF-2010 and EAF-2005 σmax. 7Li(n, d), E=9-60 MeV; compiled, compared EAF-2007 and EAF-2010 σ. 54Fe(n, p), E=2-20 MeV;compiled, compared EAF-2010 and EXFOR data.

doi: 10.3938/jkps.59.1100
Citations: PlumX Metrics


2009CA27      Nucl.Data Sheets 110, 3107 (2009)

R.Capote, M.Herman, P.Oblozinsky, P.G.Young, S.Goriely, T.Belgya, A.V.Ignatyuk, A.J.Koning, S.Hilaire, V.A.Plujko, M.Avrigeanu, O.Bersillon, M.B.Chadwick, T.Fukahori, Z.Ge, Y.Han, S.Kailas, J.Kopecky, V.M.Maslov, G.Reffo, M.Sin, E.Sh.Soukhovitskii, P.Talou

RIPL - Reference Input Parameter Library for Calculation of Nuclear Reactions and Nuclear Data Evaluations

doi: 10.1016/j.nds.2009.10.004
Citations: PlumX Metrics


2009SU11      Nucl.Technology 168, 279 (2009)

J.-Ch.Sublet, R.A.Forrest, J.Kopecky

The EAF-2007 Neutron, Deuteron, and Proton Activation Libraries

doi: 10.13182/NT09-A9195
Citations: PlumX Metrics


1993KO01      Phys.Rev. C47, 312 (1993)

J.Kopecky, M.Uhl, R.E.Chrien

Radiative Strength in the Compound Nucleus 157Gd

NUCLEAR REACTIONS 156Gd(n, γ), E=2, 24 keV; measured capture Eγ, Iγ; deduced σ(E). 157Gd deduced E1, M1 strength function, <Γγ>. Resonance averaging.

doi: 10.1103/PhysRevC.47.312
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13930.


1992BE26      Phys.Rev. C46, 945 (1992)

E.Betak, J.Kopecky, F.Cvelbar

Another Possible Manifestation of the Energy-Dependent Width of the Giant Dipole Resonance

NUCLEAR REACTIONS 130Te, 176Yb(p, γ), E ≈ 5-25 MeV; calculated σ(E). 208Pb, 141Pr(n, γ), 142Ce, 130Te(p, γ), E=3-25 MeV; calculated activation, integrated σ(E) ratio; deduced composite nuclei GDR energy dependent width possible manifestation.

doi: 10.1103/PhysRevC.46.945
Citations: PlumX Metrics


1992BE33      Phys.Rev. C46, 1276 (1992)

F.Becvar, P.Cejnar, R.E.Chrien, J.Kopecky

Test of Photon Strength Functions by a Method of Two-Step Cascades

NUCLEAR REACTIONS Nd(n, γ), E=thermal; measured γγ-sum spectra, two step cascade spectra; deduced E1 strength function, s-wave resonance average total Γγ. Different models.

doi: 10.1103/PhysRevC.46.1276
Citations: PlumX Metrics


1990KO09      Phys.Rev. C41, 1941 (1990)

J.Kopecky, M.Uhl

Test of Gamma-Ray Strength Functions in Nuclear Reaction Model Calculations

NUCLEAR REACTIONS 197Au, 143Nd, 105Pd, 93Nb(n, γ), E=low; analyzed capture data. 94Nb, 198Au, 144Nd, 106Pd deduced total s-wave Γγ.

doi: 10.1103/PhysRevC.41.1941
Citations: PlumX Metrics


1989MA11      Nucl.Phys. A492, 1 (1989)

U.Mayerhofer, T.von Egidy, P.Durner, G.Hlawatsch, J.Klora, H.Lindner, S.Brant, H.Seyfarth, V.Paar, V.Lopac, J.Kopecky, D.D.Warner, R.E.Chrien, S.Pospisil

Nuclear Structure of 198Au Studied with (n, γ) and (d, p) Reactions and Interpreted with the IBFFM

NUCLEAR REACTIONS 197Au(d, p), E=20 MeV; measured E(p), σ(E(p)). 197Au(n, γ), E=2 keV, 24 keV; measured E(γ), I(γ). 198Au deduced levels, γ-branching ratios, γ-multipolarity, J, π. Interacting boson-fermion-fermion model calculations.

doi: 10.1016/0375-9474(89)90506-X
Citations: PlumX Metrics


1988AB04      J.Phys.(London) G14, Supplement S373 (1988)

K.Abrahams, M.W.Konijnenberg, J.Kopecky, F.Stecher-Rasmussen, R.Wervelman

Meson Exchange Currents in Few-Nucleon Systems and Radiative Capture of Neutrons

NUCLEAR REACTIONS 2H(polarized n, γ), E not given; measured γ CP vs Eγ.

doi: 10.1088/0305-4616/14/S/037
Citations: PlumX Metrics


1988KO07      Phys.Lett. 205B, 215 (1988)

M.W.Konijnenberg, K.Abrahams, J.Kopecky, F.Stecher-Rasmussen, R.Wervelman, J.H.Koch

Evidence for Meson-Exchange Currents in the Radiative Thermal Neutron Capture by Deuterium Nuclei

NUCLEAR REACTIONS 2H(polarized n, γ), E=thermal; measured γ CP; deduced meson exchange current role.

doi: 10.1016/0370-2693(88)91652-8
Citations: PlumX Metrics


1987KO27      Nucl.Phys. A468, 285 (1987)

J.Kopecky, R.E.Chrien

Observation of the M1 Giant Resonance by Resonance Averaging in 106Pd

NUCLEAR REACTIONS 105Pd(n, γ), E=2, 24 keV; measured Eγ, Iγ. 106Pd deduced γ-ray strength functions. Enriched targets.

doi: 10.1016/0375-9474(87)90518-5
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22384.


1986KO16      Radiat.Eff. 94, 293 (1986)

J.Kopecky

Study of the Distribution of M1 Radiative Strength from Resonance-Averaged Neutron Data

NUCLEAR STRUCTURE 96Mo, 102Ru, 106Pd, 114Cd, 162Dy, 168Er, 176Lu, 233Th, 239U; analyzed data; deduced M1 transition strength distribution characteristics. 239U, 106Pd, 168Er, 176Lu, 233Th deduced Eγ(M1), EWSR.

doi: 10.1080/00337578608208395
Citations: PlumX Metrics


1986KO39      Radiat.Eff. 94, 293 (1986); see 1986Ko16

J.Kopecky

doi: 10.1080/00337578608208395
Citations: PlumX Metrics


1985CH08      Nucl.Phys. A436, 205 (1985)

R.E.Chrien, J.Kopecky, H.I.Liou, O.A.Wasson, J.B.Garg, S.Dritsa

Distribution of Radiative Strength from Neutron Capture by 239Pu

NUCLEAR REACTIONS 239Pu(n, γ), E=thermal-50 eV; measured Eγ, Iγ. 240Pu deduced resonances, Γγ, s-, p-wave strength functions, average level spacing.

doi: 10.1016/0375-9474(85)90196-4
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset10916.


1985KO26      Int.J.Appl.Radiat.Isotop. 36, 657 (1985)

J.Kopecky

Proton Beam Monitoring via the Cu(p, x)58Co, 63Cu(p, 2n)62Zn and 65Cu(p, n)65Zn Reactions in Copper

NUCLEAR REACTIONS, ICPND Cu(p, X)58Co, 63Cu(p, 2n), 65Cu(p, n), E=4-33 MeV; measured residual production σ(E).

doi: 10.1016/0020-708X(85)90008-0
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0333.


1984CH05      Nucl.Phys. A414, 281 (1984)

R.E.Chrien, J.Kopecky

The Nuclear Structure of 239U

NUCLEAR REACTIONS 238U(polarized n, γ), E=thermal; 238U(n, γ), E=2, 24 keV; measured Eγ, Iγ, γ CP. 239U deduced levels, J, π.

doi: 10.1016/0375-9474(84)90645-6
Citations: PlumX Metrics


1984KO29      Nucl.Phys. A427, 413 (1984)

J.Kopecky, M.G.Delfini, R.E.Chrien

Investigation of the 59Co(n, γ)60Co Reaction with Unpolarized and Polarized Neutrons

NUCLEAR REACTIONS 59Co(n, γ), (polarized n, γ), E=thermal, 24 keV; measured Eγ, Iγ, γ CP; deduced Q-value. 60Co deduced levels J, π, γ-branching. Natural unoriented targets.

doi: 10.1016/0375-9474(84)90223-9
Citations: PlumX Metrics


1983DE28      Nucl.Phys. A404, 225 (1983); Erratum Nucl.Phys. A410, 513 (1983)

M.G.Delfini, J.Kopecky, J.B.M.De Haas, H.I.Liou, R.E.Chrien, P.M.Endt

Study of the 63Cu(n, γ)64Cu Reaction

NUCLEAR REACTIONS 63Cu(n, γ), E=thermal, 2, 24 keV; measured Eγ, Iγ; deduced Q-value. 64Cu deduced levels, J, π, γ-branching. Enriched, oriented, unoriented targets.

doi: 10.1016/0375-9474(83)90548-1
Citations: PlumX Metrics


1983DE29      Nucl.Phys. A404, 250 (1983)

M.G.Delfini, J.Kopecky, R.E.Chrien, H.I.Liou, P.M.Endt

Study of the 65Cu(n, γ)66Cu Reaction

NUCLEAR REACTIONS 65Cu(n, γ), (polarized n, γ), E=thermal, 2, 24 keV; measured Eγ, Iγ, γ CP; deduced Q-value. 66Cu deduced levels, J, π, γ-branching. Enriched targets.

doi: 10.1016/0375-9474(83)90549-3
Citations: PlumX Metrics


1983TI02      Nucl.Phys. A403, 13 (1983)

T.A.A.Tielens, J.Kopecky, K.Abrahams, P.M.Endt

The Reaction 23Na(n, γ)24Na Studied with Unpolarized and Polarized Thermal Neutrons

NUCLEAR REACTIONS 23Na(n, γ), (polarized n, γ), E=thermal; measured Eγ, Iγ, γ CP; deduced (B(n)). 24Na deduced levels, γ-branching, J, π. Natural targets.

doi: 10.1016/0375-9474(83)90184-7
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset21862.


1982TI02      Nucl.Phys. A376, 421 (1982)

T.A.A.Tielens, J.Kopecky, F.Stecher-Rasmussen, W.Ratynski, K.Abrahams, P.M.Endt

Investigation of the 45Sc(n, γ) Reaction

NUCLEAR REACTIONS 45Sc(n, γ), E=thermal; measured Eγ, Iγ; deduced Q-value. 46Sc deduced levels J, π, γ-branching.

doi: 10.1016/0375-9474(82)90121-X
Citations: PlumX Metrics


1981DE04      Nucl.Phys. A352, 125 (1981)

J.De Boer, K.Abrahams, J.Kopecky, P.M.Endt

Investigation of the 31P(n(pol), γ)32P Reaction

NUCLEAR REACTIONS 31P(polarized n, γ), E=thermal; measured CP for γ-rays. 32P levels deduced J, channel spin mixing, δ.

doi: 10.1016/0375-9474(81)90563-7
Citations: PlumX Metrics


1980KO01      Nucl.Phys. A334, 35 (1980)

J.Kopecky, R.E.Chrien, H.I.Liou

Resonance Neutron Capture in 52Cr

NUCLEAR REACTIONS 52Cr(n, γ), E=thermal, 1626 eV; measured Eγ, Iγ; deduced Q. 53Cr levels deduced J. Natural, enriched targets.

doi: 10.1016/0375-9474(80)90137-2
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13918.


1980LI07      Nucl.Phys. A337, 401 (1980)

H.I.Liou, R.E.Chrien, J.Kopecky, J.A.Konter

Study of the 45Sc(n, γ) Reaction

NUCLEAR REACTIONS 45Sc(polarized n, γ), (n, γ), E ≈ 0.0253 eV, E=0.14-7.65 eV, 460.6, 1060.4, 3290, 4330 eV; measured Eγ, Iγ, γ-CP; deduced B(n). 46Sc deduced resonances, J, multipolarity, γ strength function. Oriented, unoriented targets.

doi: 10.1016/0375-9474(80)90151-7
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12725.


1980VE05      Nucl.Phys. A344, 421 (1980)

R.Vennink, J.Kopecky, P.M.Endt, P.W.M.Glaudemans

Investigation of the 56Fe(n, γ)57Fe and 58Fe(n, γ)59Fe Reactions

NUCLEAR REACTIONS 56,58Fe(n, γ), E=thermal; measured Eγ, Iγ; deduced Q. 57,59Fe deduced levels, γ-branching, J, π. Enriched, natural targets.

doi: 10.1016/0375-9474(80)90400-5
Citations: PlumX Metrics


1978VE06      Nucl.Phys. A299, 429 (1978)

R.Vennink, W.Ratynski, J.Kopecky

Circular Polarization of Neutron Capture γ-Rays from Ca, Ti, Fe and Ni

NUCLEAR REACTIONS 42Ca, 44Ca, 46Ti, 56Fe, 58Fe, 64Ni(polarized n, γ), E=th; measured γ-CP. 43Ca, 45Ca, 47Ti, 57Fe, 59Fe, 65Ni levels deduced J. Enriched targets.

doi: 10.1016/0375-9474(78)90381-0
Citations: PlumX Metrics


1977CH20      Phys.Rev.Lett. 39, 911 (1977)

R.E.Chrien, J.Kopecky

Implications for Radiative-Strength Functions from Neutron Capture in 35Cl

NUCLEAR REACTIONS 35Cl(n, γ), E ≈ 0.025, 400 eV; measured Eγ, Iγ. 36Cl deduced transitions.

doi: 10.1103/PhysRevLett.39.911
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13915.


1977CL03      Phys.Lett. 71B, 10 (1977)

C.F.Clement, A.M.Lane, J.Kopecky

Correlations in M1 Neutron Capture as Evidence for a Semi-Direct Mechanism

NUCLEAR REACTIONS 19F, 23Na, 25Mg, 27Al, 29Si, 31P, 35,37Cl, 39K, 43Ca(n, γ), (d, p); analyzed correlations between reaction types.

doi: 10.1016/0370-2693(77)90726-2
Citations: PlumX Metrics


1976SP06      Nucl.Phys. A264, 63 (1976)

A.M.J.Spits, J.Kopecky

The Reaction 35Cl(n, γ)36Cl Studied with Non-Polarized and Polarized Thermal Neutrons

NUCLEAR REACTIONS 35Cl(polarized n, γ), 35Cl(n, γ), E=thermal; measured Eγ, Iγ, γ-CP; deduced Q, polarization function R. 36Cl levels deduced γ-branching, J, π, δ. Natural targets.

doi: 10.1016/0375-9474(76)90145-7
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset20591.


1973KO16      Nucl.Phys. A215, 54 (1973)

J.Kopecky, F.Stecher-Rasmussen, K.Abrahams

A Study of the Cu(n, γ) Reaction

NUCLEAR REACTIONS Cu(polarized n, γ), E=thermal; measured γ-CP; 64,66Cu levels deduced J. Natural target.

doi: 10.1016/0375-9474(73)90100-0
Citations: PlumX Metrics


1973KO27      Nucl.Phys. A215, 45 (1973)

J.Kopecky, K.Abrahams, F.Stecher-Rasmussen

The 57Fe(n, γ)58Fe Reaction

NUCLEAR REACTIONS 57Fe(polarized n, γ), E=thermal; measured Eγ, Iγ, γ-CP; deduced Q; 58Fe levels deduced J. Enriched target.

doi: 10.1016/0375-9474(73)90099-7
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset20539.


1972KO15      Nucl.Phys. A188, 535 (1972)

J.Kopecky, K.Abrahams, F.Stecher-Rasmussen

Study of the (n, γ) Reaction in the Mass Region A = 50 - 63

NUCLEAR REACTIONS 50Cr, 52Cr, 54Fe, 60Ni, 62Ni(polarized n, γ);E= thermal; measured Eγ, Iγ, γ-CP; deduced Q. 51Cr, 53Cr, 55Fe, 61Ni, 63Ni levels deduced J. Enriched targets.

doi: 10.1016/0375-9474(72)90218-7
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset20226.


1972OP02      Phys.Lett. 39B, 204 (1972)

A.M.F.Op den Kamp, J.Kopecky, F.Stecher-Rasmussen, K.Abrahams, P.M.Endt

Interference of the Two Spin Components of the Capture State in the (n, γ) Reaction

NUCLEAR REACTIONS 39K(n, γ), E=thermal; measured γ-CP; deduced interference of 2 spin components in capture state.

doi: 10.1016/0370-2693(72)90776-9
Citations: PlumX Metrics


1972ST04      Nucl.Phys. A181, 225 (1972)

F.Stecher-Rasmussen, K.Abrahams, J.Kopecky

Circular Polarization of Neutron Capture γ-Rays from Al, Ar and Ca

NUCLEAR REACTIONS 27Al, 40Ar, 40,44Ca(polarized n, γ);E=thermal; measured γ-CP. 28Al, 41Ar, 41,45Ca levels deduced J, π. 28Al transition deduced γ-mixing. Natural targets.

doi: 10.1016/0375-9474(72)90915-3
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset20539.


1972ST05      Nucl.Phys. A181, 241 (1972)

F.Stecher-Rasmussen, K.Abrahams, J.Kopecky

A Study of the 59Co(n, γ)60Co Reaction with Polarized Thermal Neutrons

NUCLEAR REACTIONS 59Co(polarized n, γ);E=thermal; measured γ-CP. 60Co levels deduced J, π. Natural target.

doi: 10.1016/0375-9474(72)90916-5
Citations: PlumX Metrics


1972ST06      Nucl.Phys. A181, 250 (1972)

F.Stecher-Rasmussen, J.Kopecky, K.Abrahams, W.Ratynski

Circular Polarization of Neutron Capture γ-Rays from Mn, Ni, Ga and W

NUCLEAR REACTIONS 55Mn, 58,60,62Ni, 69,71Ga, 182,183,186W(polarized n, γ), E=thermal; measured γ-CP. 56Mn, 59,61,63Ni, 70,72Ga, 183,184,187W levels deduced J, π. Natural targets.

doi: 10.1016/0375-9474(72)90917-7
Citations: PlumX Metrics


1970AB09      Phys.Lett. 32B, 605 (1970)

K.Abrahams, J.Kopecky, F.Stecher-Rasmussen

Negative Energy Resonances and Potential Capture in the 59Co(n, γ) Reaction

NUCLEAR REACTIONS 59Co(polarized n, γ), E=thermal; measured γ-circular polarization. 60Co deduced negative energy resonance, level-width.

doi: 10.1016/0370-2693(70)90556-3
Citations: PlumX Metrics


1969KO05      Nucl.Phys. A127, 385 (1969)

J.Kopecky, E.Warming

Circular Polarization Measurements with a Ge(Li) Detector

NUCLEAR REACTIONS 32S, 35Cl, 48Ti, 55Mn, 56Fe, 59Co, 63Cu(polarized n, γ), E = thermal; measured γ circular polarization. 33S, 36Cl, 49Ti, 56Mn, 57Fe, 60Co, 64Cu levels deduced J, γ-mixing. Natural targets.

doi: 10.1016/0375-9474(69)90579-X
Citations: PlumX Metrics


1968HO08      Czech.J.Phys. 18B, 34 (1968)

J.Honzatko, J.Kajfosz, J.Kopecky

Mixing Ratio of the 0.34 MeV (M1+E2) Transition in 49Ti

NUCLEAR REACTIONS 48Ti(n, γ), E=thermal measured γ directional polarization correlation. 49Ti transition deduced γ-mixing ratio.


1968KA12      Nucl.Phys. A120, 225 (1968)

J.Kajfosz, J.Kopecky, J.Honzatko

Search for Time-Reversal Non-Invariance in Strong Interactions

NUCLEAR REACTIONS 48Ti(polarized n, γ), E=thermal; measured Eγ, γγ(θ). 49Ti deduced validity of time-reversal invariance. Natural target.

doi: 10.1016/0375-9474(68)90070-5
Citations: PlumX Metrics


1967WA14      Phys.Lett. 25B, 200 (1967)

E.Warming, F.Stecher-Rasmussen, W.Ratynski, J.Kopecky

Parity-Non-Conserving Internucleon Potentials Studied in the 113Cd(n, γ)114Cd Reaction

NUCLEAR STRUCTURE 114Cd; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0370-2693(67)90035-4
Citations: PlumX Metrics


1966KA14      Phys.Letters 20, 284 (1966)

J.Kajfosz, J.Kopecky, J.Honzatko

A Test for Time-Reversal Invariance in Nuclear Forces

doi: 10.1016/0031-9163(66)90366-0
Citations: PlumX Metrics


1965KO10      Nucl.Phys. 68, 449 (1965)

J.Kopecky, J.Kajfosz, B.Chalupa

Circular Polarization of Gamma-Rays Following the Capture of Polarized Neutrons on S, V, Co, Cu and Zr

NUCLEAR REACTIONS S, V, Co, Cu, Zr(polarized n, γ), E=thermal; measured Eγ, Iγ, γ-polarization. 33S, 52V, 60Co, 64Cu, 93Zr deduced J, π. Natural targets.

doi: 10.1016/0029-5582(65)90661-9
Citations: PlumX Metrics


1961UR01      Czechoslov.J.Phys. 11B, No.8, 559 (1961)

J.Urbanec, J.Kajfosz, J.Kopecky

NUCLEAR STRUCTURE 60Co; measured not abstracted; deduced nuclear properties.


1960KO07      Czechoslov.J.Phys. 10B, 119 (1960)

J.Kopecky, J.Kajfosz, J.Urbanec

Radiative Capture of Thermal Neutrons on Nucleus II

NUCLEAR STRUCTURE 68Zn, 69Zn, 67Zn, 110Ag, 108Ag, 24Na, 125Te, 124Te, 128I, 60Co; measured not abstracted; deduced nuclear properties.

doi: 10.1007/BF01557111
Citations: PlumX Metrics


1960UR02      Czechoslov.J.Phys. 10B, 275 (1960)

J.Urbanec, J.Kajfosz, J.Kopecky

The Radiative Capture of a Neutron on Sc, Fe, Cu, Mo, Cd and La Nuclei

NUCLEAR STRUCTURE 46Sc, 57Fe, 66Cu, 64Cu, 96Mo, 140La, 114Cd; measured not abstracted; deduced nuclear properties.


1959UR02      Czechoslov.J.Phys. 9, 544 (1959)

J.Urbanec, J.Kopecky, J.Kajfosz

Radiative Capture of Slow Neutrons on Atomic Nuclei


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